• Title/Summary/Keyword: HTS conductor

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The effect of non-uniform current distribution on transport current loss in stacked high-Tc superconductor tapes

  • Choi, Se-Yong;Nah, Wan-Soo;Joo, Jin-Ho;Ryu, Kyung-Woo;Lee, Byoung-Seob;Yoon, Jang-Hee;Ok, Jung-Woo;Park, Jin-Yong;Won, Mi-Sook
    • Progress in Superconductivity and Cryogenics
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    • v.14 no.2
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    • pp.16-19
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    • 2012
  • The influence of current distribution on the transport current loss in vertically stacked high-$T_c$ superconductor (HTS) tapes was evaluated. AC loss was analyzed as a function of current distribution by introducing a current distribution parameter through a numerical method (finite element analysis). AC loss under non-uniform current distribution is always higher than that for a uniformly distributed transport current in a conductor. Although the effect of non-uniformity is relatively insignificant in low transport current, AC loss increases substantially in high transport current regions as non-uniformity is enlarged. The results verify that non-uniform current distribution causes extra loss by examining the cross-sectional view of current densities in stacked conductor.

Quench/recovery test results of the YBCO coated conductors(CCs) having various stabilizer thicknesses (YBCO coated conductors(CCs)의 안정화재 두께 변화에 따른 quench/recovery 특성 분석에 관한 연구)

  • Kwon, N.Y.;Kim, H.S.;Kim, K.L.;Kim, K.J.;Yim, S.W.;Kim, H.R.;Hyun, O.B.;Lee, H.G.
    • Progress in Superconductivity and Cryogenics
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    • v.11 no.3
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    • pp.10-14
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    • 2009
  • Since a stabilizer of YBCO coated conductor (CC) plays a very important role of bypassing over-current and transferring heat generated in the moment of fault, it is one of big issues to determine the material of the stabilizer and its dimension for the high performance of the HTS power application system. Especially, in the case of a superconducting fault current limiter (SFCL), which requires it to react immediately to the occurrence of fault, characteristics of stabilizer are decisive in limiting fault current and recovering superconducting properties during and after quenching. In this paper, the quench / recovery characteristics of YBCO CCs with various thickness of stabilizer were analyzed. The quench/recovery test carried out at 20 $V_{rms}$, 5 cycles (60 Hz) and results showed that as the thickness of the stabilizer decreased, both the final approach temperature and the recovery time decreased.

A study on the current limiting characteristics and magnetic analysis of the non-inductively wound coil (타입에 따른 무유도 권선형 코일의 한류 특성연구 및 자장해석)

  • Jang, Jae-Young;Park, Dong-Keun;Chang, Ki-Sung;Na, Jin-Bae;Kim, Won-Cheol;Chung, Yood-Do;Ko, Tae-Kuk
    • Progress in Superconductivity and Cryogenics
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    • v.11 no.1
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    • pp.25-29
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    • 2009
  • To reduce the power loss in normal state, non-inductively wound high temperature superconducting (HTS) coils are used for fault current limiter (FCL) application. Non-inductively wound coils can be classified into two types: solenoid type and pancake type. These two types have different electrical and thermal and mechanical characteristics due to their winding structure difference. This paper deals with the current limiting characteristics, magnetic field analysis of the two coils. Simulation using finite element method (FEM) was used to analyze the magnetic field distribution and inductance of the coils. Short circuit test using stabilizer-free coated conductor (CC) was also carried out. We can compare the characteristics of the two types of coil by using the data obtained from simulation and short circuit test. We confirmed the feasibility of FCL application by the analysis about the characteristics of non-inductively wound coil using CC.

Estimation of the maximum magnetic field applied perpendicularity on the HTS conductor for a large scale SMES (SMES용 고온초전도 코일에 인가되는 최대 자기장의 계산)

  • Lee, Ji-Young;Lee, Seyeon;Kim, Yungil;Park, Sang Ho;Choi, Kyeongdal;Lee, Ji-Kwang;Kim, Woo-Seok
    • Proceedings of the KIEE Conference
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    • 2015.07a
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    • pp.1120-1121
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    • 2015
  • 대용량 SMES(Superconducting Magnetic Energy Storage)를 제작하기 위해서는 높은 자장특성을 가고 있는 2세대 HTS(High-Temperature Superconductor) 선재를 사용하는 것이 효율적이다. SMES의 에너지밀도를 높이기 위해서는 선재에 많은 전류를 흘려야 하는데, 수직자기장이 커지면 임계전류가 작아지는 2세대 HTS 선재의 특성상 토로이드형태의 SMES가 유리하다. SMES를 설계하기 전에 선재의 사용량을 줄이고 체적을 줄이기 위해서 정확한 설계와 평가가 필요하다. 유한요소법을 사용한 상용프로그램을 이용하여 쉽게 해석할 수 있으나 토로이드 형태의 SMES는 대칭성의 문제로 3차원 해석을 해야만 한다. 그러나 2차원 해석에 비해 여러 가지 제약조건이 따르며 해석 시간이 많이 소요된다. 본 논문에서는 이러한 문제점을 해결하기 위해 분석적이고 통계적으로 고온 초전도 코일에서 작용하는 최대 수직자장을 결정하는데 이해하기 쉽고 효율적으로 계산하는 방법을 제시했다. 본 논문에서는 싱글펜케이크코일의 크기에 따른 최대 자장값을 계산하였고 싱글펜케이크코일이 토로이드형태로 배치된 토로이드 모델에서 주변코일이 싱글펜케이크코일의 미드포인트에 미치는 자장값을 계산하여 두 계산값을 합하는 방식으로 최대 자기장을 계산하였다. 이 방법은 현저한 시간단축과 효율적인 설계를 할 수 있는 새로운 계산 방법으로 기존 FEM을 사용해 걸리는 시간에 비해 1/1000정도의 시간단축을 할 수 있었다.

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Charateristics analysis of the joining of YBCO 2G HTS wire (YBCO 2G 선재간 접합 특성 연구)

  • Chang, Ki-Sung;Park, Dong-Keun;Yang, Seong-Eun;Ahn, Min-Cheol;Jo, Dae-Ho;Kim, Hyoun-Kyu;Lee, Hai-Gun;Ko, Tae-Kuk
    • Proceedings of the KIEE Conference
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    • 2006.07b
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    • pp.741-742
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    • 2006
  • This paper deals with an efficient superconducting joint method between 2G high superconducting(HTS) wire, YBCO coated conductor(CC). Recently CC is one of the most promising superconducting wire due to high n-value and critical current independency from external magnetic field. It is expected to be used many superconducting application such as fault current limiter, persistent current system and cable etc. In most HTS applications, superconducting magnet is used, and it is necessary to joint between superconducting wire to fabricate superconducting magnet system. A CC tape used in this research consists of copper stabilizer, silver layer, YBCO layer, buffer and substrate. Direct joint using soldering method was inefficient due to resistance of copper, then copper lamination is removed by chemical etching method to reduce resistance between CC tapes. Jointed tapes were fabricated and tested. Transport current through jointed area and induced voltage were measured to characterize the I-V curve. Resistance between CC wire using chemical etching was compared with resistance of direct jointed tapes using soldering method in this paper.

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Superconductivity recovery of vacuum annealed HTS GdBCO CC

  • You, Jong Su;Yang, Jeong Hun;Song, Kyu Jeong
    • Progress in Superconductivity and Cryogenics
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    • v.24 no.3
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    • pp.41-46
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    • 2022
  • The superconducting properties of high temperature superconducting (HTS) GdBCO coated conductor (CC) tape (Ag/GdBCO/Buffer-layers/Stainless Steel) were investigated, specifically a series of samples prepared by vacuum heat treatment (200℃ to 600℃), using a Quantum Design PPMS-14. The critical current density Jc value was obtained by applying the modified Bean model to the irreversible magnetization ∆Mirr(H) data which was estimated from the magnetization M(H) loop. The reduction rates of lnJc and Tc values according to the increase of the vacuum annealing temperature Tan were d(lnJc)/dTan = - 0.016 A/(cm2∙℃) and dTc/dTan = - 0.24, respectively. We examined the effect of recovery temperature Tre (475℃ to 700℃) and recovery duration time t (0.5 h to 24 h) on the restoration of previously completely lost superconductivity in samples that subsequently received heat treatment in an O2 gas flow space. All samples were fully restored to superconductivity by heat treatment in an O2 gas flow space. The recovery temperatures Tre (475℃ to 700℃) and recovery duration times t (0.5 h to 24 h) were both independent of the superconductivity recovery characteristics.

STRATEGIC RESEARCH AT ORNL FOR THE DEVELOPMENT OF ADVANCED COATED CONDUCTORS: PART - I

  • Christen, D.K.;Cantoni, C.;Feenstra, R.;Aytug, T.;Heatherly, L.;Kowalewski, M.M.;List, F.A.;Goyal, A.;Kroeger, D.M.
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2002.02a
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    • pp.339-339
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    • 2002
  • In the RABiTS approach to coated conductor development, successful (both economic and technological) depends on the refinement and optimization of each of three important components: the metal tape substrate, the buffer layer(s), and the HTS layer. Here we will report on the ORNL approach and progress in each of these areas. - Most applications will require metal tapes with low magnetic hysteresis, mechanical strength, and excellent crystalline texture. Some of these requirements are competing. We report on progress in obtaining a good combination of these characteristics on metal alloys of Ni-Cr and Ni-W. - The deposition of appropriate buffer layers is a crucial step. Recently, base research has shown that the presence of a stable sulfur superstructure present on the metal surface is needed for the nucleation and epitaxial growth of vapor-deposited seed buffer layers such as YSZ, CeO$_2$ and SrTiO$_3$. We report on the details and control of this superstructure for nickel tapes, as well as recent results for Cu and Ni-13%Cr. - Processes for deposition of the HTS coating must economically provide large values of the figure-of-merit for conductors, current x length. At ORNL, we have devoted efforts to a precursor/post-annealing approach to YBCO coatings, for which the deposition and reaction steps are separate. We describe motivation for and progress toward developing this approach. - Finally, we address some issues for the implementation of coated conductors in real applications, including the need for texture control and electrical stabilization of the HTS coating.

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Long length HTS coated conductor by RABiTS PLD method (RABiTS PLD 법을 이용한 장선 박막형 고온초전도선재)

  • Ko, Rock-Kil;Kim, Ho-Sup;Ha, Hong-Soo;Yang, Joo-Sang;Park, Yu-Mi;Song, Kyu-Jeong;Oh, Sang-Soo;Park, Chan;Kim, Young-Cheol
    • Proceedings of the KIEE Conference
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    • 2005.07c
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    • pp.1841-1843
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    • 2005
  • 냉간 압연과 열처리 공정을 통해 2축 배향성을 가지는 금속 기판 위에 산화물 박막을 중착 시켜 같은 정도의 2축 배향성을 갖도록 제조된 RABiTS template 위에 YBCO 초전도체를 PLD 방법으로 증착하여 YBCO coated conductor 선재를 제조하였다. RABiTS template은 $NiW/Y_2O_3/YSZ/CeO_2$ 구조로 DC reactive sputtering와 PLD 방법에 의해 증착되었다. 모든 공정은 reel-to-reel 방식의 연속 공정으로 이루어졌다. 1m와 10m급의 장선 고온초전도선재를 제조하고, 이에 대한 전기적 특성과 초전도 및 다층 산화물 완충층에 대한 결정성, 표면 특성에 대한 분석을 수행하였다. 그 결과 1m 길이에서 end-to-end 107A와 10.6m 길이에서 end-to-end 51A의 임계 전류를 획득하였다. 제조된 박막형 선재의 초전도 층과 다층의 산화물 완충층 모두 금속 기판의 결정성을 그대로 유지하면서, epitaxial하게 성장하였으며, 최종 YBCO의 in-plane FWHM 값은 > $9^{\circ}$를 유지하였다.

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Long length HTS coated conductor by RABiTS-PLD method (RABiTS-PLD 법을 이용한 장선 박막형 고온초전도선재)

  • Ko, Rock-Kil;Kim, Ho-Sup;Ha, Hong-Soo;Yang, Joo-Sang;Park, Yu-Mi;Song, Kyu-Jeong;Oh, Sang-Soo;Park, Chan;Kim, Young-Cheol
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2005.07a
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    • pp.50-51
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    • 2005
  • 냉간 압연과 열처리 공정을 통해 2축 배향성을 가지는 금속 기판 위에 산화물 박막을 증착 시켜 같은 정도의 2축 배향성을 갖도록 제조된 RABiTS template 위에 YBCO 초전도체를 PLD 방법으로 증착하여 YBCO coated conductor 선재를 제조하였다. RABiTS template은 NiW/$Y_2O_3$/NSZ/$CeO_2$ 구조로 DC reactive sputtering와 PLD 방법에 의해 증착되었다. 모든 공정은 reel-to-reel 방식의 연속 공정으로 이루어졌다. 1m와 10m급의 장선 고온초전도선재를 제조하고, 이에 대한 전기적 특성과 초전도 및 다층 산화물 완충층에 대한 결정성, 표면 특성에 대한 분석을 수행하였다. 그 결과 1m 길이에서 end-to-end 107 A와 10.6m 길이에서 end-to-end 51A의 임계 전류를 획득하였다. 제조된 박막형 선재의 초전도 층과 다층의 산화물 완충층 모두 금속 기판의 결정성을 그대로 유지하면서, epitaxial하게 성장하였으며, 최종 YBCO의 in-plane FWHM 값은 > $9^{\circ}$를 유지 하였다.

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Design of the Magnetic Core Reactor for the connection to the Power System of DC Reactor Type High Temperature Superconducting Fault Current Limiter (DC 리액터형 고온초전도한류기의 전력계통 연계를 위한 자기철심리액터의 설계)

  • 임대준;배덕권;김호민;이찬주;윤경용;윤용수;고태국
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2002.02a
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    • pp.322-325
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    • 2002
  • In this paper, the power-linking device connecting the high-Tc super-conducting(HTS) coil to the power system in the DC reactor type three-phase high-Tc superconducting fault current limiter (SFCL) has been designed. This design was triggered from the concept that the magnetic energy could be exchanged into the electrical energy each other. Ferromagnetic material is used as the path of magnetic flux. The device mentioned above was named Magnetic Core Reactor(MCR). MCR was designed to minimize the voltage drop caused by copper loss. The current density of the conductor was 1.3 A/mm$^2$ and % voltage drop was 2%.

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